IndexForces & FieldsTee

Decay Dancer

Weak Nuclear Force / Beta Decay Physics

\[n \to p + e^{-} + \bar\nu_e\]
Regular price $28.99 USD
Regular price Sale price $28.99 USD
Sale Sold out

Inside some nuclei, a neutron quietly changes its identity. In beta-minus decay the weak force turns a neutron into a proton, emitting an electron and an antineutrino. Decay Dancer wears it in pixel art on a unisex tee. The physics panel below has the equation, every symbol and the sources.

Color
Size

Size guide S–5XL · inches

Shipping calculated at checkout by destinationMade to order, ships in 2–5 business days

Details

Size & fitS–5XL

Unisex heavy cotton (Gildan 5000), classic fit.

Unisex tee size chart, inches
SizeWidthLengthSleeve
S182815.1
M202916.5
L223018
XL243119.5
2XL263221
3XL283322.4
4XL303423.7
5XL323525

Measurements in inches, ±1.5 in tolerance.

ShippingBy destination

Shipping calculated at checkout by destination. Printed to order for you.

Delivery times & where we ship

Returns & replacements21 days

Every item is printed to order, so we can’t accept returns or exchanges for change of mind, or if you ordered the wrong size or colour.

Print defect, misprint, damage or the wrong item? We’ll send a free replacement, or a refund if you prefer. Report it within 21 days of delivery with a photo; no need to send it back.

Full refund & replacement policy

The physics

A neutron, left alone, does not stay a neutron.

Inside a stable nucleus a neutron can last indefinitely. Set it free and on average it lasts a little under fifteen minutes before it becomes a proton, an electron, and an electron antineutrino. Underneath, one of its down quarks turns into an up quark by way of a \(W^{-}\) boson, a particle about eighty-five times heavier than the neutron itself, which exists here only as a fleeting intermediate and immediately becomes the electron and the antineutrino. Changing a quark's flavour this way is something only the weak force does.

The accounting is exact. A neutron outweighs a proton plus an electron by 0.782 MeV of rest energy, and the decay products share exactly that. Early measurements found the electrons coming out with a spread of energies below that maximum, as if energy were going missing. In 1930 Wolfgang Pauli proposed an unseen neutral particle carrying the difference. Enrico Fermi built a theory of beta decay around it in 1934 and gave it its name. Clyde Cowan and Frederick Reines detected it in 1956. The next year Chien-Shiung Wu's experiment with cobalt-60 showed that beta decay does not look the same in a mirror.

The strange part is the clock. Trap ultracold neutrons in a bottle and count how many survive: 878.4 ± 0.5 seconds. Measure a neutron beam instead and count the protons that come out: about nine seconds longer. Both methods are careful work, and they still disagree. Nobody yet knows why.

Decay Dancer is the neutron mid-turn: same mass number, new identity, something invisible leaving at the edge of the frame.

Equations

\[n \to p + e^{-} + \bar\nu_e\]
\[d \to u + W^{-} \to u + e^{-} + \bar\nu_e\]
\[Q = \left(m_n - m_p - m_e\right)c^{2} \approx 0.782\ \text{MeV}\]
Symbols
SymbolMeaningUnit
\(n, p\) neutron, proton —
\(e^{-}\) electron —
\(\bar\nu_e\) electron antineutrino —
\(d, u\) down, up quark —
\(W^{-}\) virtual W boson —
\(m_n, m_p, m_e\) neutron, proton, electron masses \(\mathrm{kg}\)
\(Q\) kinetic energy shared by the decay products (neutrino mass neglected; quoted in MeV) \(\mathrm{J}\)